US1753330A - Metering device - Google Patents

Description

H. E. BRAGG April 8, 1930.

METERING DEVI CE Filed Sept. 22, 1928 Fla.

//vv/v rm HERBERT 55mm;

Patented Apr. 8, 1930 I UNITED STATES.

PATENT oF ica HERBERT E. BRAGG, OF EAST ORANGE, NEw JERSEY, AssIeNoETo BELL TELEPHONE LABORATORIES, INCORPORATED, OF NEW YORK, N. Y., A CORPORATION OF NEW YORK METERING nEvIcE a Application filed September 22, 1928. Seflal'No. 307,756.

This invention relates to voltage indicating devices and more particularly to such devices as are employed to meter transient peak voltages.

In studying the effects of and remedying the evils produced by peak voltages 1t is highly desirable that a means for measuring and indicating such voltages be available and that such means be in the nature of a simple, compact structure, easily manipulated and continuous and accurately dependable; Heretofore, I when investigating the phenomena of peak voltages it was necessary to set up an elaboratecircuit arrangement involving the use of vacuum tubes and the capacitive and inductive variables exigent upon the use of such tubes, which resulted in a long, tedious series of tests and frequently terminated in false measurements. v

It is the object of this invention to rovide a compact, highly dependable porta .le device for indicating and measuring peak voltages, which may be quickly installed and readily adjusted to satisfy varying conditions.

This object is attained in accordance with a feature of the invention by utilizing the cathode glow of a gas filled discharge tube as a means for directly indicating the value of the voltage impressed on the anode-cathode circuit of the tube.

The invention contemplates the use of a calibrated tubeor reservoir containing neon,

so that by merely securing the terminals of the tube to the terminals across which the voltage is to be measured, a direct reading in volts may be made.

The invention 'Will be readily understood from the following description made with reference to the accompanying drawingsin which Fi 1 is a two electrode gas filled dis- 7 charge tu e and Fig. 2 is a four electrode as filled discharge tube, both of which invo ve the principles underlying this invention. Like numerals indicate similar elements throughout the drawings.

Referring to Fig. 1, a glass tube or reservoir 5 is provided with a re-entrant seal 6 through which one end of a cathode 7, preferably of fine nickel wire extends. The other end of the cathode 7 is sealed to the top of the glass tube 5 in any suitable manner and is so located that the cathode 7 assumes a position corresponding to the longitudinal axis of the tube. An annular anode 8, also preferably of nickel, is located near the base of the tube 5 and is secured thereto in any suitable manner. Lead-in wires-9 and 10 are provided for the cathode 7 and anode 8 respectively, and are ada ted to beconnected to an external circuit voltage. A constant resistance element 12 of relatively hi h resistance compared to the impedance 0 the circuit'producing the un- 'nected to the terminals of the circuit producmg the'unknown voltage in any well known manner, whereupon the rare gas in the reservoir 5 ionizes and the cathode 7 assumes a glow due tothe gaseous discharge, the length of glow on the cathode bein a. function of thevoltage impressed across t e anode-cathode circuit. It is believed unnecessary in this description to enter into the theory of the ionization of gases,-as all phases of this phenomenon are well known to those skilled in the art. It may be well however, to note that a gas discharge tube of this type has what is generally known as acritical or breakdown which represents an unknown voltage, so that for any voltage lower than this critical value no gas ionization takes p ace.

Depending upon the value of the voltage impressed on the anode-cathode circuit, the length of the glow along the cathode wire 7 vanes and the glass tube 5 being callbratedin the two electrode type as depicted in, Fig. 1,

electrodes 20 and 21 accordingly, are

there is an inherent lag in the ionization of the gas when the anode-cathode circuit is associated with a voltage supply. In measuring ordinary peak voltages this lag does not detract from the accurateness of the tube as a meter, but when transient voltages are to be measured, the length of the cathode glowwould not be an exact indication of the impressed voltage owing to the fact that the transient voltage is not maintained sufiiciently long to permit the gas to fully ionize and a correct reading to be taken. .The auxilifllary rnished and a secondary current supply 22 is connected across their terminals through the resistance element 24, It is to be understood that the voltage impressed on the auxiliary electrodes is just below the critical or breakdown voltage of the tube. So that when a. transient voltage is to be measured, the tube shown in Fig. 2 is employed and the key 23 is actuated to cause an initial gas ionization which overcomes the inherent lag. The same result may be accomplished by eliminating the auxiliary electrodes and connecting an external potential in series with the main anode or cathode in the proper direction, but

of a value just'below the breakdown voltage V of the tube. In any case the unknownpotential is a function of the length of the cathode glow "andthe tube can be calibrated to read directly in volts. What is claimed is:

1. In combination a direct reading voltage indicator comprising a gas filled reservoir a pair of electrodes located'therein, a calibrated scale on said reservoir, one of s id electrodes constituting a central axis .for said reservoir and means'exclusive of said electrodes for producing an initial ionization of the gas in said reservolr.

2. In combination a direct reading voltage indicator comprising a gas filled reservoir, a

trodes to cause ionization of the gas in said reservoir and produce a glow on one of said electrodes, the length of which is a function of the unknown voltage, a source of power having a terminal voltage less than the breakdown voltage of said gas filled reservoir and a pair of electrodes associated with said sourceof power and adapted to produce an initial ionization of the gas within said reservo1r. V

In witness whereof, I hereunto subscribe my name this 20th day of September, 1928.

, HERBERT E. BRAGG.

pair of electrodes located therein, a calibrated scale on said reservoir, one of said electrodes constituting apentral axis for said reservoirand a circuit including a pair of electrodes electrically independent of said first mentioned electrodes, for producing an initial ionization of the gas in said reservoir.

3, In combination, a direct reading voltage Indicator comprising a gas filled calibrated reservoir, a pair of electrodeslocated therein, one of said electrodeslnonstituti a central axis for said resermir, as'ource 0 unknown voltage adapted-tabs 'nn'pressed on said

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